Problem 84
Question
\(\bullet$$\bullet\) A ray of light traveling in a block of glass \((n=1.52)\) is incident on the top surface at an angle of \(57.2^{\circ}\) with respect to the normal in the glass. If a layer of oil is placed on the top surface of the glass, the ray is totally reflected. What is the maximum possible index of refraction of the oil?
Step-by-Step Solution
Verified Answer
The maximum possible index of refraction of the oil is approximately 1.28.
1Step 1: Understand the Problem
A ray of light inside a glass block with an index of refraction \(n_{glass} = 1.52\) is incident at an angle \(\theta_{glass} = 57.2^{\circ}\) to the normal of the surface. An oil layer is added on top and the light is totally internally reflected. We must find the maximum index of refraction \(n_{oil}\) for this scenario.
2Step 2: Apply Snell's Law for Total Internal Reflection
For total internal reflection at the interface between the glass and the oil, the critical angle \(\theta_c\) must satisfy:\[\sin(\theta_c) = \frac{n_{oil}}{n_{glass}}\]Since the light is totally internally reflected, an incident angle equal to or greater than \(\theta_c\) means \(\theta_{glass} = \theta_c\).
3Step 3: Solve for the Critical Angle
The critical condition for total internal reflection is:\[sin(\theta_{glass}) = \frac{n_{oil}}{n_{glass}}\]Hence:\[\sin(57.2^{\circ}) = \frac{n_{oil}}{1.52}\]Calculate \(\sin(57.2^{\circ})\).
4Step 4: Calculate \(\sin(57.2^{\circ})\)
Using a calculator, find:\[sin(57.2^{\circ}) \approx 0.8415\]This value will be used in the next step to find \(n_{oil}\).
5Step 5: Solve for Maximum Index of Refraction of Oil
Substitute \(\sin(57.2^{\circ})\) into the equation:\[0.8415 = \frac{n_{oil}}{1.52}\]Rearrange to solve for \(n_{oil}\):\[n_{oil} = 0.8415 \times 1.52\]Calculate this value.
6Step 6: Final Calculation
Perform the multiplication:\[n_{oil} \approx 1.2791\]Hence, the maximum possible index of refraction of the oil is approximately \(1.28\).
Key Concepts
Snell's LawCritical AngleIndex of Refraction
Snell's Law
Snell's Law is a fundamental principle that describes how light behaves when it moves between different media. It states that the ratio of the sine of the angles of incidence and refraction is equal to the ratio of the indices of refraction of those two media. Mathematically, it is expressed as:
This law helps us predict how light will bend at the boundary between two different materials. For example, if light travels from air (\( n = 1.00 \)) into water (\( n = 1.33 \)), Snell's Law can determine how much it will bend. Understanding this principle is crucial for tackling problems where light behaves in unusual ways, such as through lenses or over transitions into different media.
In our exercise, Snell's Law helps to establish the conditions under which total internal reflection occurs. When light transitions from glass to oil, using this law will ensure that the conditions for total internal reflection are correctly identified by balancing the indices.
- \( n_1 \sin(\theta_1) = n_2 \sin(\theta_2) \\)
This law helps us predict how light will bend at the boundary between two different materials. For example, if light travels from air (\( n = 1.00 \)) into water (\( n = 1.33 \)), Snell's Law can determine how much it will bend. Understanding this principle is crucial for tackling problems where light behaves in unusual ways, such as through lenses or over transitions into different media.
In our exercise, Snell's Law helps to establish the conditions under which total internal reflection occurs. When light transitions from glass to oil, using this law will ensure that the conditions for total internal reflection are correctly identified by balancing the indices.
Critical Angle
The critical angle is a specific angle of incidence at which light traveling from one medium to another less dense medium ends up being reflected entirely back into the original medium. This phenomenon only occurs if the light is moving from a medium with a higher index of refraction to one with a lower index.
Here's how it works:
In our original exercise, the angle exceeds the critical angle, causing total internal reflection at the boundary of glass and oil. Knowing this critical angle helps us determine the maximum possible index of refraction for the oil, setting up the scenario where this reflection condition holds true.
Here's how it works:
- If \( \theta > \theta_c \): total internal reflection happens.
- \( \sin(\theta_c) = \frac{n_{low}}{n_{high}} \)
In our original exercise, the angle exceeds the critical angle, causing total internal reflection at the boundary of glass and oil. Knowing this critical angle helps us determine the maximum possible index of refraction for the oil, setting up the scenario where this reflection condition holds true.
Index of Refraction
The index of refraction, sometimes called the refractive index, is a measure of how much light slows down as it enters a material. Each material has its own unique refractive index, and this value is crucial for explaining many optical phenomena.
Here’s what you should know:
Understanding the refractive indices of different materials enables us to apply Snell's Law correctly and analyze conditions like total internal reflection. For instance, in the optical setup with glass and oil, the task is to find the maximum refractive index of the oil, ensuring that light does not just incidentally pass through but is reflected inwardly. Using steps from the solution, we realize the calculation is key to optimizing how the light behaves at these interfaces.
Here’s what you should know:
- A higher index means light travels slower in that medium and bends more when it enters the material.
- It’s a dimensionless number, typically greater than 1, signifying that light always travels slower in a medium compared to a vacuum.
Understanding the refractive indices of different materials enables us to apply Snell's Law correctly and analyze conditions like total internal reflection. For instance, in the optical setup with glass and oil, the task is to find the maximum refractive index of the oil, ensuring that light does not just incidentally pass through but is reflected inwardly. Using steps from the solution, we realize the calculation is key to optimizing how the light behaves at these interfaces.
Other exercises in this chapter
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